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| United States Patent | 5396807 |
| Link to this page | http://www.wikipatents.com/5396807.html |
| Inventor(s) | Dowty; Earl L. (Katy, TX);
Hatton; Gregory J. (Kingwood, TX) |
| Abstract | The gas flow rate and liquid flow rate of a two phase fluid flow are
determined by passing the fluid flow down an inclined pipe to stratify the
flow. The fluid pressure, temperature and density are measured along with
the liquid density. The differential pressure is measured to determine the
dynamic head of the fluid. These measurements are used together to
determine the gas flow rate and the liquid flow rate. |
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Title Information  |
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Drawing from US Patent 5396807 |
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Means to determine liquid flow rate with gas present |
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| Publication Date |
March 14, 1995 |
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| Filing Date |
June 14, 1994 |
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Title Information  |
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Description  |
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BACKGROUND OF THE INVENTION
1. The Field of the Invention
The present invention pertains to a means and method for determining the
liquid flow rate and gas flow rate of a fluid mixture containing these two
phases.
2. The Prior Art
A fundamental measurement required in many industries is the measurement of
the flow of liquids and gases and a determination of their respective
rates of flow. Special consideration is being directed, by sectors of the
oil industry interested in the development of sub sea production
technology, to liquid rate meters which are passive (i.e. have no moving
parts) and offer high reliability, availability and proven performance.
The innovative recognition of gas-liquid stratification that occurs in a
downwardly inclined section of flow line has led to several means for
measuring the liquid and gas flow rates. These means have generally
included active components, i.e. components with moving parts. Example of
this type of apparatus can be found in U.S. Pat. Nos. 4,660,414;
4,760,742; 5,048,348; 5,127,272; and 5,195,380, all owned by the common
assignee and the disclosures of which are incorporated herein by
reference. The present invention is also based on the use of a downwardly
inclined section of a flow line, but is totally passive and makes use of
components of proven reliability, availability and performance.
SUMMARY OF THE INVENTION
The liquid and gas flow metering device of the present invention is
completely passive (i.e. has no moving parts), operates over a broad range
of flow rates and conditions, is suitable for high operating pressures
(e.g. greater than 3600 psia), introduces negligible pressure losses, can
be used subsurface as well as on the surface, and has a self draining
configuration which does not trap fluids or entrained solids when the
system is shut in.
BRIEF DESCRIPTION OF THE DRAWINGS
The present invention will be described, by way of example, with reference
to the accompanying drawings in which:
FIG. 1 is a side elevation, partially broken away, of a gas flow and liquid
flow metering device according to the present invention; and
FIG. 2 is a representative cross section used to explain certain
computations in the present invention.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT
An embodiment of an apparatus for performing the present invention is shown
in schematic form in FIG. 1. The apparatus 10, which is an inclined
stratifying device of the type mentioned above, is connected between pipes
12, 14 by known flange coupling means 16,18. The stratifying portion
includes integral riser pipe 20 and downwardly inclined pipe 22 of known
internal diameter and cross sectional configuration. Pressure measuring
means 24 and temperature sensing means 26 are shown connected to the riser
to sense the pressure and temperature, respectively, of the fluid mixture
in the pipe. A first density measuring means 28 is mounted on the inclined
pipe substantially normal to the surface of the liquid flowing
therethrough to determine the average density of the fluid stream in the
inclined pipe segment 22. A second density measuring means 30 is mounted
in the inclined pipe transverse to the axis of the pipe, but positioned to
be below the surface of the liquid flowing therein, to determine the
density of the liquid, with any entrained gas, flowing in the lower
portion of the inclined pipe. Differential pressure sensing means 32, with
probes above and below the flowing liquid, determine the dynamic head of
the liquid, with any entrained gas, flowing in the lower portion of the
inclined pipe 22.
The following detailed discussion describes how the liquid flow and gas
flow rates are determined using the present invention. The measurement of
pressure and temperature, with the knowledge of thermodynamic properties
of the fluid mixture's liquid and gas components, enable the depth of the
liquid, with any entrained gas, in the inclined flow line section to be
calculated from the average density measurement utilizing the following
equation:
##EQU1##
in which:
1=depth of the liquid (with entrained gas).
D=inside diameter of the pipe.
.rho..sub.avg =average density of fluid flowing down the inclined pipe
section, measured by means 28 in a plane oriented perpendicular to the
axis of the inclined pipe.
.rho..sub.gas =density of the gas at the pressure and temperature of the
flowing fluid.
.rho..sub.liq-g =density of liquid (with entrained gas) measured via means
30 in a horizontal plane oriented perpendicular to pipe at an elevation
immediately upstream of the dynamic head probe inlet.
The cross sectional area of the inclined section occupied by the liquid,
containing some entrained gas, can now be determined if the configuration
of the cross section is known. For example, consider an inclined section
with a circular cross-sectional area. This is illustrated in FIG. 2. The
angle .alpha., which indicates the radial portion of the inclined section
occupied by the liquid with entrained gas, is determined from the
equation:
##EQU2##
and the area occupied by the liquid with entrained gas is:
##EQU3##
The velocity of the liquid with entrained gas, V.sub.liq-g, is determined
by the measurement of the dynamic head via means 32 from the relationship:
.DELTA.P.sub.dyn =1/2.rho..sub.liq-g V.sub.liq-g.sup.2
in which .DELTA..rho..sub.dyn denotes the dynamic head measurement.
Rearranging gives
##EQU4##
Therefore, the volumetric liquid rate (with entrained gas), Q.sub.liq-g is
Q.sub.liq-g =A.sub.liq-g V.sub.liq-g
Correcting for the gas entrained in the liquid,
##EQU5##
in which
X.sub.gas-entr ="entrained" gas fraction
Q.sub.liq =corrected volumetric liquid flow rate.
.rho..sub.liq =density of liquid at temperature and pressure of flowing
fluid.
Similarly, the total gas fraction, X.sub.gas, is obtained from:
##EQU6##
and the total gas rate, Q.sub.gas, is defined by
##EQU7##
All measurements are made by industry accepted passive means.
The design evolved from considering alternative ways to determine liquid
flow rate using liquid stratification within downwardly inclined flow line
sections. The use of devices, such as pitot tubes, to determine the
dynamic head of the flow stream is a classic measurement that has been
proven an accurate way to determine the velocity of a flowing stream.
The present invention may be subject to many modifications and changes,
which will occur to those skilled in the art, without departing from the
spirit or essential characteristics thereof. Therefore the present
embodiment should be considered in all respects as illustrative and not
restrictive of the scope of the present invention as defined by the
appended claims.
* * * * *
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Description  |
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